Device for dispersing light pulses of which the spectral amplitude is programmable

ABSTRACT

Device for dispersion of light pulses of an optical beam (Fi) constituted by two dispersive prisms (P 1 , P 2 ), with the same vertex angle (α), mounted head to tail, the optical input surface of the first prism (P 1 ) being parallel to the optical output surface of the second prism (P 2 ), the distance (L) separating said optical input surface of the first prism (P 1 ) and said optical output surface of the second prism (P 2 ) being adjustable, given that the material constituting at least one of said first and second prisms (P 1 , P 2 ) is an acousto-optic material allowing for acousto-optic interaction between said optical beam and an acoustic beam, the acoustic wave of said acoustic beam generating, in at least one of said first and second prisms (P 1 , P 2 ), an integrated deflective Bragg cell.

BACKGROUND OF THE INVENTION

1. Field of the Invention

This invention relates to a device for dispersion of light pulses programmable in spectral amplitude.

2. Description of the Prior Art

In general, it is known that there are numerous devices for dispersing brief light pulses. One of them, proposed for the first time by R. L. Fork et al, “Negative dispersion using pairs of prisms”, published in Optics Letters, May 1984, consists of using a train of two identical reversed prisms (the input surface of the first prism is parallel to the output surface of the second prism).

In the example shown in FIG. 1, describing the prior art relating in particular to the device cited above, two prisms P₁, P₂, having the same vertex angle a, are arranged head to tail, the input surface of said prism P₁ is parallel to the output surface of said prism P₂, the distance separating them being L; the output surface of said first prism P₁ is consequently parallel to the input surface of said prism P₂, the distance separating them being d; the projection of the vertex of said prism P₂ on the input surface of said prism P₁ is separated by H from the vertex of said prism P₁.

The modification of the dispersion characteristic associating the delay time with the optical wavelength is performed by modifying the distance L that separates the input and output surfaces of the prisms Pi, P₂; the modification of the dispersion characteristic can also be performed by modifying the distance H that separates the vertices of the two prisms P₁, P₂.

SUMMARY OF THE INVENTION

It appears that all of these devices for dispersing brief light pulses do not make it possible to modify, over time, the relative amplitude of the various wavelengths of said light pulses.

The invention is therefore intended more specifically to overcome this disadvantage. It proposes a device for dispersing light pulses of an optical beam constituted by two dispersive prisms, with the same vertex angle, mounted head to tail, the optical input surface of the first prism being parallel to the optical output surface of the second prism, the distance separating said optical input surface of the first prism and said optical output surface of the second prism being adjustable, given that the material constituting at least one of said first and second prisms is an acousto-optic material allowing for acousto-optic interaction between said optical beam and an acoustic beam, the acoustic wave of said acoustic beam generating, in at least one of said first and second prisms, an integrated deflecting Bragg cell. In such a device, the various optical wavelengths have been spatially separated from one another transversely by the dispersion of the prisms.

The acousto-optic Bragg cell, of which the axis is almost perpendicular to the light rays, diffracts, selectively in amplitude, the various optical wavelengths according to the signals applied to the transducer of said Bragg cell.

The diffracted waves are eliminated from the device according to the invention; only the non-diffracted waves, of which the amplitude according to the optical wavelength has been made programmable by the acousto-optic interaction, are involved in the dispersion device.

Advantageously, the incident optical beam is perpendicular or almost perpendicular to the input and output surfaces, respectively, of said first and second prisms, and is polarised perpendicularly to the edges of the prisms.

In addition, the vertex angle of said first and second prisms is such that the light radiation of said optical beam corresponds to a wavelength at the centre of the spectrum, i.e. under the Brewster incidence relative to the input and output surfaces, respectively, of said first and second prisms.

Advantageously, the material constituting at least one of said first and second prisms is a tellurium dioxide crystal (TeO₂)-type acousto-optic material of which the surface associated with a piezoelectric transducer Ta forms an angle of less than 15 degrees with the optical axis [001] of said tellurium dioxide crystal (TeO₂).

In addition, said piezoelectric transducer Ta generates an acoustic wave of which the amplitude and/or the frequency are programmed as a function of time; the signals applied to said piezoelectric transducer Ta are provided by a generator, associated with a calculator that displays the amplitude and frequency parameters desired as a function of time.

BRIEF DESCRIPTION OF THE DRAWINGS

An embodiment of the invention is described below, by way of a non-limiting example, with reference to the appended drawings, in which:

FIG. 1 is a diagrammatic representation of a device according to the prior art,

FIG. 2 is a diagrammatic representation of a device according to the invention,

FIG. 3 is a representation of curves with an ordinary and an extraordinary index of the tellurium dioxide crystal (TeO₂) in the plane containing the optical axes [110] and [001],

FIG. 4 is a representation of the characteristics of relative variation in the group delay time as a function of the optical wavelength,

FIG. 5 is a representation of the characteristics of relative variation in the height of the acoustic column as a function of the optical wavelength, and

FIG. 6 is a representation of the characteristic of the acoustic frequency to be applied as a function of the optical wavelength.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

In the example shown in FIG. 1, two prisms P₁, P₂, with the same vertex angle a, are arranged head to tail, the input surface of said prism P₁ is parallel to the output surface of said prism P₂, the distance separating them being L; the output surface of said first prism P₁ is consequently parallel to the input surface of said prism P₂, the distance separating them being d; the projection of the vertex of said prism P₂ on the input surface of said prism P₁ is separated by H from the vertex of said prism P₁.

An optical incident beam Fi is diffracted by the prism P₁, which resulting diffraction is represented by three optical paths having a wavelength λ₁, λ₂, on each side of a central wavelength λ₀, which paths are again diffracted in the second prism P₂; at the output of the second prism P2, the three optical paths having a wavelength λ₀, λ₁ , λ₂, are spatially separated from one another and parallel to the incident beam Fi, the dispersion associating the delay time with the optical wavelength being dependent on the distance L and/or the distance H.

It should be noted that the variation in the delay time can be positive or negative depending on the geometric characteristics of the device.

In the example shown in FIG. 2, two truncated prisms P₁, P₂, with the same vertex angle α, are arranged head to tail, the input surface of said prism P₁ is parallel to the output surface of said prism P2, the distance separating them being L; the output surface of said first prism P₁ is consequently parallel to the input surface of said prism P₂, the distance separating them being d; the distance between the vertices of the prisms P₁, P₂, defined perpendicularly to the distance L is equal to H.

An optical incident beam Fi is perpendicular to the input and output surfaces, respectively, of said prisms P₁, P₂; the polarisation of light is perpendicular to the edges of the prisms; the material constituting said prisms P₁, P₂, is a birefringent acousto-optic tellurium dioxide crystal TeO₂; the angle at the vertex of said prisms P₁, P₂, is such that the central wavelength of the light pulse bandwidth comes out of the output surface of the prism P₁ and enters the input surface of the prism P₂, under the Brewster angle.

Thus, in the vicinity of the output surface of the first prism P₁, the wavelengths, represented by the optical paths λ₀, λ₁, λ₂, are spatially separated from one another, so as to arrive at the input surface of the second prism P₂, which, after refraction in the second prism P₂, are mutually parallel and normal to the output surface of the second prism P₂.

If:

L is the distance separating the input and output surfaces, respectively, of prisms P₁, P₂,

H is the distance between the vertices of said prisms P₁, P₂, defined perpendicularly to the distance L,

α is the angle at the vertex of prisms P₁, P₂,

θ is the diffraction angle between the prisms P₁, P₂, according to the wavelength, defined with respect to the normal to the output and input surfaces, respectively, of the prisms P₁, P₂,

c is the speed of light,

n is the extraordinary index of the tellurium dioxide crystal, and N (N=n−λ.dn/dλ), is the extraordinary group index of the tellurium dioxide crystal, in the direction of the incident light rays, the delay time of group t_(R) of the light between the input and output surfaces, respectively, of prisms P₁, P₂, is defined by the following equation: $\frac{c\quad t_{R}}{L} = {\frac{1}{G} \cdot \left\lbrack {\frac{1}{\cos\quad\theta} + {N \cdot \left( {G - {\cos\quad\alpha} - {\sin\quad{\alpha \cdot \tan}\quad\theta}} \right)}} \right\rbrack}$ with:   sin   θ = n ⋅ sin   α α + θ₀ = π/2

θ₀ being the diffraction angle, for the central wavelength λ₀, which satisfies the Brewster condition, i.e.: tan θ₀ =n(λ₀), and

G being a geometric parameter equal to the ratio of said distance L to said distance d, defined by the following equation: $G = {\frac{L}{d} = \left( {{\cos\quad\alpha} - {{\frac{H}{L} \cdot \sin}\quad\alpha}} \right)^{- 1}}$

In the example shown in FIG. 2, a piezoelectric transducer Ta, constituting the Bragg cell, is integrated with the base surface of the prism P₂, which base surface forms an angle θ_(A) of several degrees with the optical axis [001] of the tellurium dioxide crystal, i.e. 5 degrees, for example.

The acoustic height Δh is defined as being the distance that separates the optical paths of wavelength λ₁, λ₂, on each side of the central wavelength λ₀, in the second prism P₂.

Thus:

θ_(A) is the angle of the base of the prism P₂ with respect to the optical axis [001] of the crystal; θ_(A) is also the angle of the acoustic wavelength vector with the optical axis [110] of the crystal,

θ_(i) is the angle of the incident beam Fi with respect to the optical axis [110] of the crystal,

θ₀ is the angle of the optical path of wavelength λ₀ with respect to the normal to the output surface of the first prism P₁, and

θ_(a) is the angle of inclination of the acoustic energy beam with respect to the base of the second prism P₂.

In the example shown in FIG. 3:

the axis of abscissas is represented by the optical axis [110] of the tellurium dioxide crystal,

the axis of ordinates is represented by the optical axis [001] of the tellurium dioxide crystal,

the curve of ordinary index no is represented by the circle C_(O) with centre O,

the curve of extraordinary index n is represented by the ellipse C₁ of which the small axis, according to 001, corresponds to the radius n₀ of said circle C_(O), and the large axis, according to 110, has the value n_(e).

The deflection occurs from the extraordinary incident rays to ordinary diffracted rays in the plane containing the optical axes [001] and [110] of the tellurium dioxide crystal; for the central wavelength, the acoustic wave vector is approximately tangential to the ordinary index curve so as to provide the largest possible spectral band for the diffraction of extraordinary incident rays to ordinary rays, thus:

the optical incident wave vector k_(i) is represented by the vector OB,

the optical diffracted wave vector k_(d) is represented by the vector OA,

the acoustic wave vector K is represented by the vector AB,

θ_(i) is the angle of the optical incident wave vector k_(i) with respect to the optical axis [110],

θ_(d) is the angle of the optical diffracted wave vector k_(d) with respect to the optical axis [110],

θ_(A) is the angle of the acoustic wave vector K with respect to the optical axis [110].

Under these conditions, the angle θ_(i) of the optical incident wave vector k_(i) with respect to the optical axis [110], is associated with the angle θ_(A) of the base of the prism P₂ with respect to the optical axis [001], by the following equation: sin(θ_(i)+θ_(A))=n ₀(λ₀)/n(λ₀)

n is associated with the ordinary n₀ and extraordinary n_(e) indices on the optical axis [110], by the following equation: $n = \frac{n_{0}n_{e}}{\sqrt{{n_{0}^{2}\cos^{2}\theta_{i}} + {n_{e}^{2}\sin^{2}\theta_{i}}}}$ and n₀ and n_(e) are given as a function of the wavelength by the Sellmeier equations, namely: $n_{0} = {\sqrt{1 + \frac{2.5838\quad\lambda^{2}}{\lambda^{2} - 0.01801} + \frac{1.1566\quad\lambda^{2}}{\lambda^{2} - 0.06959}}\quad{and}}$ $n_{e} = \sqrt{1 + \frac{2.8228\quad\lambda^{2}}{\lambda^{2} - 0.01801} + \frac{1.5416\quad\lambda^{2}}{\lambda^{2} - 0.06922}}$ For example, if λ₀ is equal to 0.8 μm:

n₀=2.226,

n_(e)=2.373, and

if θ_(A) is equal to 50:

θ_(i)=82.36°,

n=2.229,

θ₀=65.83°,

α=24.16°,

θ_(a)=49.43°.

In the example shown in FIG. 4, the characteristics of relative variation in the group delay time as a function of the optical wavelength are shown.

If t_(R0) is the group delay time for the central wavelength λ₀ equal to 0.8 μm, the variation: c.(t_(R)−t_(R0))/L is shown as a function of the optical length λ for two values of H/L, L being the distance separating the input and output surfaces, respectively, of the prisms P₁, P₂, H being the distance between the vertices of said prisms P₁, P₂, defined perpendicularly to the distance L, namely: the curves C₁, C₂, respectively for H/L=1.01 and for H/L=1.13.

The height Δh of the acoustic column in the second prism P₂, as indicated above, is given around the central wavelength λ₀.

The difference h−h₀ is defined by the following equation: $\frac{h - h_{0}}{L} = {\left( {{\cos\quad\alpha} - {\frac{H}{L}\sin\quad\alpha}} \right)\left\lbrack {\frac{\sin\left( {\theta - \alpha} \right)}{\cos\quad\theta} - \frac{\sin\left( {\theta_{0} - \alpha} \right)}{\cos\quad\theta_{0}}} \right\rbrack}$ given that:

α is the angle at the vertex of prisms P₁, P₂,

θ₀ is the angle of the optical path of wavelength λ₀ with respect to the normal to the output surface of the first prism P₁, and

θ is the angle of the optical path of wavelength λ with respect to the normal to the output surface of the first prism P₁.

In the example shown in FIG. 5, the characteristics of relative variation in the acoustic column height as a function of the optical wavelength are shown.

The variation: (h−h₀)/L is shown as a function of the optical wavelength λ for two values of H/L, L being the distance separating the input and output surfaces, respectively, of the prisms P₁, P₂, H being the distance between the vertices of said prisms P₁, P₂, defined perpendicularly to the distance L, namely: the curves C₁, C₂, respectively for H/L=1.01 and for H/L=1.13.

The total length l of the tellurium dioxide crystal passed through by light at the central wavelength λ₀ is given by the following equation: $\frac{l}{L} = \left( {{\frac{H}{L}\sin\quad 2\alpha} - {\cos\quad 2\alpha}} \right)$

The frequencies to be applied to the piezoelectric transducer Ta are given by the following equation: f=√{square root over ((615² cos² θ_(A)+2100² sin² θ_(A)).)}√{square root over ((n ² −n ₀ ²))}/λ

In the example shown in FIG. 6, the characteristic of acoustic frequency f_(A) to be applied as a function of the optical wavelength function λ defined for θ_(A) is equal to 5 degrees (curve C).

For example, for an optical bandwidth of 100 nm, a length L of 56 cm, a height H of 56 cm,

the variation in the group delay time is 4.5 picoseconds,

the total length l of crystal passed through by light is 50 mm,

the area of the height Δh of the acoustic column on which the wavelengths of the incident beam Fi are distributed is 20 mm, and

the frequency domain to be applied to the acoustic transducer is between 75 and 90 MHz.

Thus, the number of points for programming spectral amplitude of the device according to the invention, defined as being the ratio of the area of the height Δh of the acoustic column on which the wavelengths are distributed, to the diameter of the incident beam Fi is, in this case, 20 points for an incident beam Fi diameter of 1 mm.

Advantageously, the amplitude and/or the frequency of the acoustic wave generated by said piezoelectric transducer Ta are programmed as a function of time; the signals applied to said piezoelectric transducer Ta are provided by a generator, associated with a computer that displays the desired frequency and amplitude parameters as a function of time. 

1. Device for dispersion of light pulses of an optical beam constituted by two dispersive prisms, with the same vertex angle, mounted head to tail, the optical input surface of the first prism being parallel to the optical output surface of the second prism, the distance separating said optical input surface of the first prism and said optical output surface of the second prism being adjustable, wherein the material constituting at least one of said first and second prisms is an acousto-optic material allowing for acousto-optic interaction between said optical beam and an acoustic beam, the acoustic wave of said acoustic beam generating, in at least one of said first and second prisms, an integrated deflective Bragg cell, said Bragg cell, of which the axis is almost perpendicular to said optical beam, diffracts, selectively in amplitude, the various wavelengths of said optical beam according to the characteristics of said acoustic beam, thus generating non-diffracted optical waves and diffracted optical waves, said diffracted waves being eliminated, the amplitude of said non-diffracted waves is programmable according to the optical wavelength by said acousto-optic interaction.
 2. Device according to claim 1, wherein the optical incident beam is perpendicular or almost perpendicular to the input and output surfaces, respectively, of said first and second prisms, and is polarised perpendicularly to the edges of said prisms.
 3. Device according to claim 1, wherein the angle at the vertex of said first and second prisms is such that the light radiation of said optical beam corresponding to a wavelength at the centre of the spectrum, i.e. under the Brewster incidence, relative to the output and input surfaces, respectively, of said first and second prisms.
 4. Device according to claim 1, wherein the material constituting at least one of said first and second prisms is a tellurium dioxide crystal-type acousto-optic material of which the surface associated with a piezoelectric transducer forms an angle of less than 15 degrees with the optical axis [001] of said tellurium dioxide crystal.
 5. Device according to claim 1, wherein said piezoelectric transducer generates an acoustic wave of which the amplitude and/or the frequency are programmed as a function of time; the signals applied to said piezoelectric transducer are provided by a generator, associated with a computer that displays the desired frequency and amplitude parameters as a function of time. 